The charged particles produced in the O18+C12 reaction at 16.7 MeV/nucleon have been detected using the GARFIELD+RCo apparatus at Laboratori Nazionali di Legnaro and compared with the transport code antisymmetrized molecular dynamics (AMD) followed by gemini++ as afterburner. To our knowledge, it is the first time that this model is applied to a nuclear reaction between light nuclei at so relatively low bombarding energy. The general agreement between experimental data and model is very good for fragments with Z≥10, assuming a fusion process source, and for intermediate fragments (Z=3,4). A discrepancy in the relative cross section of the different reaction mechanisms has been pointed out for fragments with 4<10 as the model seems to produce less dissipative reactions.
Performance of the antisymmetrized molecular dynamics transport model for low energy reactions: Comparison with experimental results for O18+C12 at 16.7 MeV/nucleon / Baldesi, L., Barlini, S., Stefanini, A.A., Camaiani, A., Piantelli, S., Casini, G., Ciampi, C., Cinausero, M., Cicerchia, M., Dell'Aquila, D., Domenichetti, L., Fabris, D., Frosin, C., Gozzelino, A., Lombardo, I., Marchi, T., Moretto, S., Mengarelli, A., Olmi, A., Pasquali, G., et al.. - In: PHYSICAL REVIEW C. - ISSN 2469-9985. - ELETTRONICO. - 109:(2024), pp. 064618.0-064618.0. [10.1103/physrevc.109.064618]
Performance of the antisymmetrized molecular dynamics transport model for low energy reactions: Comparison with experimental results for O18+C12 at 16.7 MeV/nucleon
Baldesi, L.;Barlini, S.;Stefanini, A. A.;Camaiani, A.;Piantelli, S.;Frosin, C.;Olmi, A.;Pasquali, G.;
2024
Abstract
The charged particles produced in the O18+C12 reaction at 16.7 MeV/nucleon have been detected using the GARFIELD+RCo apparatus at Laboratori Nazionali di Legnaro and compared with the transport code antisymmetrized molecular dynamics (AMD) followed by gemini++ as afterburner. To our knowledge, it is the first time that this model is applied to a nuclear reaction between light nuclei at so relatively low bombarding energy. The general agreement between experimental data and model is very good for fragments with Z≥10, assuming a fusion process source, and for intermediate fragments (Z=3,4). A discrepancy in the relative cross section of the different reaction mechanisms has been pointed out for fragments with 4<10 as the model seems to produce less dissipative reactions.
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